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Figure 14.

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Description of the numerical testbed use for the trombone in the continuous and discrete time. Transfer functions A, B, C, D, T and R are given in equations X, from which transfer functions A ˆ $ {\hat {A}} $, B ˆ $ {\hat {B}} $, C ˆ $ {\hat {C}} $ and D ˆ $ {\hat {D}} $, T ˆ $ {\hat {T}} $ and R ˆ $ {\hat {R}} $ are deduced using the bilinear transform: z s . t . | z | < 1 $ \forall z\in {\mathbb {C}}\,\mbox {s.t.}\, |z|\lt 1 $, s = 2 f s 1 z 1 1 + z 1 $ s = 2f_s\frac {1 - z^{-1}}{1 + z^{-1}} $, and given in equations (23a)–(23f), using κ = r 0 2 π ν c ( θ 0 ) c 0 $ \kappa = \frac {r_0}{2\pi \nu _c(\theta _0)\,c_0} $.

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